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BULETINUL INSTITUTULUI POLITEHNIC DIN IAŞI

buletinul institutului politehnic din iaşi - Universitatea Tehnică ...

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108 Vlad Marţian et al<br />

that all the components are constant, whereas in reality all these characteristics<br />

are dependent of the SOC, and the dicharge current. The circuit diagram can be<br />

seen in the Fig. 2.<br />

Fig. 2 – Thervein model.<br />

2.3. Non linear Dynamic Model<br />

A more realistic model has been created by extending the Thervein<br />

model. This new model takes into account the nonlinearities in the components<br />

of the Thervein model. As we said earlier the internal resistance of the battery<br />

R+R 0 and the open circuit voltage E 0 are dependent on the SOC of the battery,<br />

and also on the temperature T of the battery.<br />

Since we are interested in how the temperature of the battery changes in<br />

time we will use a modification of this later model, which can be seen in a<br />

simplified version in Fig. 3.<br />

In this model different form Thervein model we have included the<br />

internal resistance in the overvoltage resistance, for simplification purpose, and<br />

the internal resistance R and the open circuit voltage E 0 are dependent on some<br />

function of SOC.<br />

Fig. 3 – Non linear dynamic model.<br />

3. Modeling Implementation<br />

If we want to know how the current and the voltage in the battery are<br />

modified in time we have to solve a system of equations that include first order<br />

differential equations and also algebraic equations. Doing it by hand it takes a<br />

long time, and if one of the parameter is changed we will have to do it again.

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